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How to go from detector reading to dose to media
Burlin cavity theory:
f
Q
= d·S
w,det
+(1-d) · [μ
en
/ρ]
w
,
det
D
w
= M · α ·k
i
· f
Q
Bragg Gray cavity
: Ionisation chambers in High Energy X-ray
Beams
Burling cavity:
High density detectors such as diodes, MOSFET,
diamonds for High Energy X-ray beams